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2. Dioda
As implies by its name diode is the vacuum tube with 2 electrode, cathode and plate.
Sir J.A. Fleming (1849-1945) a British scienties developed diode on  1904.


Simplified structure and schema of diode seen on figure 7 above.
Cathode put on the centre of diode  surrounded by plate and heater inserted inside cathode.
When cathode heated by heater, electrons will move from cathode to plate and produce plate current.
To get a clear idea about how diode works let us observe 3 situations as follows :
 
 
 

- Dioda supplied by zero voltage
- Dioda supplied by negative voltage
- Dioda supplied by positive voltage

Diode Supplied by zero voltage
When there is no voltage difference between plate and cathode, heated electrons from cathode could never have enough energy to reach plate, those electrons will start to accumulate near by cathode forming electrons cloud. This is known as space charge. At this situation there will be no plate current.

 
 

Dioda supplied by  negative voltage

If plate is made negative with respect to cathode, the negative charge from plate will push back the electron  to cathode so the heated electron can not reach plate and still no current indication appear at the amperemeter.
 
 
 
 
 
 
 

Dioda supplied by positive voltage

If plate is made positive with respect to plate, the positive charge from plate will attract heated electron from catahode to reach plate and generate plate current. As the plate voltage increase up the plate current will also increase.
Based on the diode property we have discused above, which it can only flow plate only at certain voltage supply, so diode is applicable for current rectifier application.
 
 
 
 

 Dioda Plate Characteristic
The most important diode characteristic is the plate characteristic, it shows the coorelation between plate voltage and plate current.

Test circuit to achieve plate characteristic and the example of plate characteristic seen on Figure 11 above.
Heater voltage supplied to filament to heat diode until it reach certain temperataure (T1) and then plate voltage (Eb) increased up from 0 until it reach maximum permisible diode plate voltage.
Plate current (Ib) will increase up as the plate voltage increased, but when plate voltage reach a certain value plate current standstill although the plate voltage still increased up. This point known as saturation point.
But if diode temperature  increased up until it reach other higher temperature (T2), the increment of diode voltage will follow back the increment of plate current. This situation tells us that  the change of diode temperature can influence it capability to flow current.

Dioda Resistance
We have seen that plate current flowing through a vacuum diode varies as the plate voltage is changed. Threrefore diode may be considered as having internal resistance that limit the amount of plate current flow. This internal resistance offered by diode is known as its plate resistance. The resistance is not the same for direct current as for the alternating current. Accordingly like any vacuum tube, diode has two types resistance namely dc plate resistance and ac plate resistance.
DC plate resistance is the resistance offered by diode to direct current. To get the clear idea about dc resistance let see Figure 12A bellow

Figure 12.A shows the graph to measure DC plate resistance.  At  point P of the curve  the plate voltage is OA and the corresponding plate current is OB, then the DC plate resistance  Rb is given by
Rb  =   OA / OB
As the plate characteristic is not a straight line, therefore DC plate resistance is not constant but depend upon operating point. So regarding to the diode real  application DC plate resistance must be determined at the actual operaating point.
AC plate resitance offered by diode to alternating current  and defined as The ratio of a small change in plate voltage across a diode to the resulting change in plate current.
Figure 12.B shows us  the way to measure AC plate resistance. According to the definition of AC plate resistance, the ac plate resistance rb is given by rb = BC/YZ
As tubes are generally used with AC voltage than DC voltage so the ac plate resistance is more important than DC plate resistance.

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